MR method and MR device for determining the position of microcoil

• US 6,087,831 A
• Filed: 02/17/1998
• Issued: 07/11/2000
• Est. Priority Date: 02/20/1997
• Status: Expired due to Fees

• Current Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Original Assignee: US Philips Corporation (Koninklijke Philips N.V.)
• Inventors: Weiger, Markus, Aldefeld, Bernd, Bornert, Peter
• Primary Examiner(s): ARANA, LOUIS M
• Application Number:
  US09/024,630
• Time in Patent Office: 875 Days
• Field of Search: 324/318, 324/322, 324/306, 324/312, 324/307, 324/309, 600/422, 600/423, 600/424
• US Class Current: 324/307
• CPC Class Codes: G01R 33/285 Invasive instruments, e.g. catheters or biopsy needles, specially adapted for tracking, guiding or visualization by NMR

Abstract

The invention relates to an MR method and an MR device for determining the position of at least one microcoil (11, 12) which is provided in or on an object (1) to be examined which is situated in an examination zone. During the acquisition of microcoil MR signals (S), at least one variable magnetic gradient field acts on the examination zone, so that the k space is scanned at scanning points (k_x (t_i), k_y (t_i)). The position (x, y) of the microcoil (11, 12) is determined from at least three scanning values (S(t_i)) of a microcoil MR signal and the associated scanning points (k_x (T_i), k_y (t_i)) for example by solving a system of equations formed from these values. The MR method can be used for various scanning modes of the k space, and the acquisition of the microcoil MR signals (S) does not require any MR sequences other than the MR sequences required for determining the nuclear magnetization distribution in the examination zone.

Claims

1. A magnetic resonance (MR) method for determining the position of at least one microcoil which is provided in or on an object to be examined which is situated in an examination zone, the method comprising:

scanning k-space at known scanning points in k-space by generating at least one variable magnetic gradient field acting on the examination zone,

measuring values of microcoil MR signals at at least three of the known scanning points in k-space, and

determining position values of the microcoil directly and without Fourier transformation from at least three measured values of the microcoil MR signal and from the k-values of the associated known scanning points in k-space.

2. An MR method as claimed in claim 1, wherein the step of determining position values further comprises

determining the phase values of at least three measured values of the microcoil MR signal, and

finally determining further the position values of the microcoil from the at least three determined phase values and the k-values of the associated known scanning points in k-space.

3. An MR method as claimed in claim 2, wherein the step of finally determining further the position values from phase values further comprises

forming an error function from difference values between a respective determined phase value and a phase characteristic value formed from the k-values of the associated known scanning points in k-space and the position values of the microcoil, and

determining values of the error function for different position values in order to minimize the error function.

4. The method of claim 3 wherein the error function depends on a sum of squares of the difference values.

5. An MR method as claimed in claim 1, wherein the step of finally determining the position values of the microcoil further comprises minimizing an error function formed from equations describing the respective relationship between a measured value of the microcoil MR signal, the k-values of the associated known scanning points in k-space and the position values searched for the microcoil.

6. An MR method as claimed in claim 5, wherein the error function is formed from difference values between a respective measured value of the microcoil MR signal and a signal characteristic value formed from the k-values of the associated known scanning points in k-space and the position values of the microcoil, and wherein the error function is minimized by calculating its value for different position values.

7. The method of claim 6 wherein the error function depends on a sum of squares of the difference values.

8. An MR method as claimed in claim 1, wherein position values a previous position of the microcoil or a direction of movement of the microcoil are taken into account in order to determine the position of the microcoil.

9. An MR method as claimed in claim 1, wherein the position of the microcoil is determined from two or three mutually independent equations which describe the respective relationship between a measured value of the microcoil MR signal, the k-values of the associated known scanning points in k-space and the position values searched for the microcoil.

10. An MR method as claimed in claim 1, wherein a receiving coil system detects MR signals in order to determine the nuclear magnetization distribution in the examination zone, and wherein at the same time the microcoil detects MR signals.

11. The method of claim 1 wherein the step of scanning k-space further comprises scanning according to a spiral method, or an echo planar imaging method, or a radial method, or a spin-warp method.

12. The method of claim 1 wherein the position values of the microcoil are determined from three measured values of the MR microcoil signal.

13. A magnetic resonance (MR) device comprising:

means for scanning k-space at known scanning points in k-space by generating at least one variable magnetic gradient field acting on the examination zone,

a receiving coil system for receiving MR signals,

at least one microcoil for measuring microcoil MR signals at least three of the known scanning points in k-space, and

means for determining the position values of the microcoil directly and without Fourier transformation from at least three measured values of the microcoil MR signal and from the k-values of the associated known scanning points in k-space.